d Review A REVIEW OF TISSUE SUBSTITUTES FOR ULTRASOUND IMAGING MARTIN O. CULJAT,* yz{ DAVID GOLDENBERG,* x PRIYAMVADA TEWARI,* y and RAHUL S. SINGH* z{ * Center for Advanced Surgical and Interventional Technology (CASIT), UCLA, Los Angeles, CA; y Department of Bioengineering, UCLA, Los Angeles, CA; z Department of Surgery, UCLA, Los Angeles, CA; x Department of Psychobiology, UCLA, Los Angeles, CA; and { Department of Electrical and Computer Engineering, UCSB, Santa Barbara, CA, USA (Received 30 July 2009; revised 3 February 2010; in final form 22 February 2010) Abstract—The characterization and calibration of ultrasound imaging systems requires tissue-mimicking phan- toms with known acoustic properties, dimensions and internal features. Tissue phantoms are available commer- cially for a range of medical applications. However, commercial phantoms may not be suitable in ultrasound system design or for evaluation of novel imaging techniques. It is often desirable to have the ability to tailor acoustic properties and phantom configurations for specific applications. A multitude of tissue-mimicking materials and phantoms are described in the literature that have been created using a variety of materials and preparation tech- niques and that have modeled a range of biological systems. This paper reviews ultrasound tissue-mimicking mate- rials and phantom fabrication techniques that have been developed over the past four decades, and describes the benefits and disadvantages of the processes. Both soft tissue and hard tissue substitutes are explored. (E-mail: [email protected]) Ó 2010 World Federation for Ultrasound in Medicine & Biology. Key Words: Tissue substitute, Tissue mimicking, Tissue equivalent, Phantom, Soft tissue, Hard tissue. INTRODUCTION Tissue phantoms have been used for characterization and calibration of ultrasound imaging systems since the 1960s. Phantoms are also used to compare the performance of ultrasound systems for training of ultrasound technicians, for comparison to computer models and to assist in the development of new ultrasound transducers, systems or diagnostic techniques. The advantage of phantoms is that idealized tissue models can be constructed with well-defined acoustic properties, dimensions and internal features, thereby simplifying and standardizing the imaging environment. Phantoms are composed of tissue-mimicking mate- rials, with the majority of phantoms having a simple homogeneous internal structure. Simple or complex targets are sometimes embedded within phantoms to mimic internal structures or to serve as characterization targets. Phantoms that accurately mimic heterogeneous organs or organ systems are often referred to as anthropo- morphic phantoms. The term tissue substitute encom- passes both phantoms and tissue-mimicking materials. Phantoms and anthropomorphic phantoms are avail- able commercially, mimicking many tissues organs and organ systems. Commercial phantoms range in price from hundreds to thousands of dollars and are often preferred for training and calibration of ultrasound systems. However, commercial phantoms are typically designed for broad markets and specific applications, and are not customizable. For this reason, customized design and fabrication of tissue phantoms is required for more specialized applications requiring tailored properties or dimensions, or when seeking to reduce cost. This paper reviews many of the materials and tech- niques used to prepare both soft and hard tissue- mimicking materials and phantoms, focusing primarily on those developed for traditional ultrasound imaging rather than those developed specifically for elasticity imaging (elastography), Doppler (string phantoms) or alternate ultrasound techniques such as high-intensity focused ultrasound (HIFU). Many of the relevant acoustic properties and measurements are first discussed, followed by common materials and preparation techniques used to develop general soft tissue phantoms. The subsequent sections focus on the development of specific soft tissue phantoms and on the materials and techniques used to develop hard tissues phantoms. This paper is intended to allow the ultrasound researcher to better understand the Address correspondence to: Martin Culjat, Ph.D., CHS BH-826, 650 Charles E. Young Dr. S, Los Angeles, CA 90095. E-mail: [email protected]861 Ultrasound in Med. & Biol., Vol. 36, No. 6, pp. 861–873, 2010 Copyright Ó 2010 World Federation for Ultrasound in Medicine & Biology Printed in the USA. All rights reserved 0301-5629/$–see front matter doi:10.1016/j.ultrasmedbio.2010.02.012
13
Embed
A Review of Tissue Substitutes for Ultrasound Imaging - McMaster
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Ultrasound in Med. & Biol., Vol. 36, No. 6, pp. 861–873, 2010Copyright � 2010 World Federation for Ultrasound in Medicine & Biology
Printed in the USA. All rights reserved0301-5629/$–see front matter
asmedbio.2010.02.012
doi:10.1016/j.ultr
d Review
A REVIEW OF TISSUE SUBSTITUTES FOR ULTRASOUND IMAGING
MARTIN O. CULJAT,*yz{ DAVID GOLDENBERG,*x PRIYAMVADA TEWARI,*y and RAHUL S. SINGH*z{
*Center for Advanced Surgical and Interventional Technology (CASIT), UCLA, Los Angeles, CA; yDepartment ofBioengineering, UCLA, Los Angeles, CA; zDepartment of Surgery, UCLA, Los Angeles, CA; xDepartment of Psychobiology,
UCLA, Los Angeles, CA; and {Department of Electrical and Computer Engineering, UCSB, Santa Barbara, CA, USA
(Received 30 July 2009; revised 3 February 2010; in final form 22 February 2010)
A650 Cmculja
Abstract—The characterization and calibration of ultrasound imaging systems requires tissue-mimicking phan-toms with known acoustic properties, dimensions and internal features. Tissue phantoms are available commer-cially for a range of medical applications. However, commercial phantoms may not be suitable in ultrasoundsystem design or for evaluation of novel imaging techniques. It is often desirable to have the ability to tailor acousticproperties and phantom configurations for specific applications. A multitude of tissue-mimicking materials andphantoms are described in the literature that have been created using a variety of materials and preparation tech-niques and that have modeled a range of biological systems. This paper reviews ultrasound tissue-mimicking mate-rials and phantom fabrication techniques that have been developed over the past four decades, and describes thebenefits and disadvantages of the processes. Both soft tissue and hard tissue substitutes are explored. (E-mail:[email protected]) � 2010 World Federation for Ultrasound in Medicine & Biology.
nique developed by Madsen et al. (1998) was altered to
mimic prostate tissue (D’Souza et al. 2001). Agarose-
based prostate phantoms were developed that included
water, agarose, lipid molecules, proteins, thimerosal and
glass beads. The concentrations of agarose and glass
beads were increased to increase the attenuation of the
material. Several other materials were further added to
accommodate MRI, including ethylenediamine tetraacetic
acid and Cu21 to control the longitudinal and transverse
(T1 and T2, respectively) relaxation times.
Sinus cavity phantomsDoppler ultrasound has been proposed as a technique
to diagnose sinusitis, because the viscosity of sinus fluid is
a known indicator of the presence of an infection (Jansson
et al. 2005). One group used agar with graphite powder to
construct an anthropomorphic sinus phantom using
a mold created from a human cranium. Water-glycerol
solutions with varying viscosities were used to mimic
mucous and serous fluids in the sinus (Jansson et al.
2005). A more recent study by the same group used
bovine cortical bone to cover the graphite and agar
phantom, and used milk as the fluid mimic (Jonsson
et al. 2008). Milk was selected because of the presence
of natural scattering particles.
Skeletal muscle phantomsSkeletal muscle has acoustic properties that are close
to those of average soft tissue (Table 1); therefore, many
of the general soft tissue substitute formulations can be
used to generate materials that mimic skeletal muscle.
One group briefly described a skeletal muscle phantom
that featured a gelatin-based material (Edmonds et al.
1985) and another described an agarose-based technique
for use as a multimodal phantom (D’Souza et al. 2001).
Fig. 2. Low melting point metal alloy core and container used toshape vascular flow phantoms of agar and konjac/carrageenangel (Meagher et al. 2007). The gel was poured into the containerand the metal alloy was melted away by placing the phantom in
a hot water and potassium chloride bath.
868 Ultrasound in Medicine and Biology Volume 36, Number 6, 2010
Both techniques treated skeletal muscle as an isotropic
material.
Vascular phantomsA number of techniques have been developed to
acoustically model vascular structures, with the majority
focusing on large arteries, such as the carotid artery and
coronary artery. Vascular phantoms can be grouped into
three general categories: basic vascular phantoms with
a simple tubular structure; walled vascular phantoms,
which have a closer resemblance to the arteries; and
wall-less phantoms, which do not have tubing separating
the tissue-mimicking and blood-mimicking materials.
Real vessels harvested from cadavers have also been
used as phantoms in many studies (Kerber and Heilman
1992; Dabrowski et al. 1997, 2001). However, because
of their limited longevity and variable geometries and
flow patterns, excised vascular tissues are poor models.
Basic vascular phantoms have been made from PVA
(Nadkarni et al. 2003; Schaar et al. 2005). A combination
of 10% PVA solution with 0.75% enamel paint followed
by two freeze-thaw cycles was found to have properties
similar to human vascular tissue (Nadkarni et al. 2003).
This technique allowed the elasticity to be varied by
changing the concentrations of PVA to model both
healthy and diseased tissue. Another basic vessel phantom
was constructed using latex rubber tubing to mimic the
femoral artery, and by mounting the tubing within a gelatin
filled frame to mimic the adjacent soft tissue (Zhang and
Greenleaf 2006). Another group used a rubber ring with
wires attached to the outer surface to provide fiducial
markers (Kawase et al. 2007).
Walled vascular phantoms have been built to better
understand the onset of vascular diseases using ultra-
sound. A rigid model of carotid artery bifurcation was
created by injecting water-soluble jeweler’s wax into an
acrylic mold (Bharadvaj et al. 1982). Another group adap-
ted this technique by using lead-cored nylon as fiducial
markers, acrylic and high-density polyethylene as a protec-
tive housing and layers of agar-based materials to improve
visibility of the fiducial markers in the ultrasound image
(Frayne et al. 1993). The blood-mimicking fluid was
created from machine tool–cutting fluid, as discussed
earlier. A later version replaced the agar gels with solid
polyester to improve durability but caused beam distor-
tions and artifacts because of an increased impedance
mismatch (Smith et al. 1994). In another study examining
vascular plaques in the carotid arteries, arterial phantoms
were made using an acrylic rod within a box that was filled
with a solidified mixture of agar, glycerol, distilled water
and sigma cells (Anthony and Aaron 2002; Landry and
Fenster 2002). Plaques were created by pouring the
same mixture with a reduced concentration of sigma
cells into stainless steel molds and embedding the
plaques into the acrylic rod. A water and glycerol
mixture was used as the blood substitute.
Wall-less vascular phantoms have been used for
evaluation of Doppler ultrasound systems. These phan-
toms are better suited to Doppler flow studies, because
image distortion that typically results from tube walls is
reduced (Patterson and Foster 1983; Rickey et al. 1995).
Homogeneous vascular phantoms were constructed
using the European Commission agar-based technique,
which also featured water, glycerol, benzalkonium chlo-
ride, Al2O3 and SiC (Teirlinck et al. 1998; Ramnarine
et al. 1999; Tortoli et al. 2006). A mixture of pure
water, glycerol, orgasol particles and a surfactant served
as the blood mimic (Ramnarine et al. 1999; Tortoli et al.
2006). This phantom was reported to have good
longevity and durability to flow (Ramnarine et al. 1999),
but the agar-based tissue-mimicking material was subject
to splitting at the bifurcation apex (Meagher et al. 2007).
To combat this problem, one group replaced the agar
material with konjac and carrageenan gels (Fig. 2)
(Meagher et al. 2007).
Multi-organ phantomsAnthropomorphic phantoms have been developed
that mimic complete organ systems rather than individual
tissues or organs. Madsen et al. (1980) developed a torso
section using water-alcohol–based gelatin with n-propa-
nol and various test objects to mimic the kidneys, liver,
tumors, cysts and bones. Another group designed
a multi-organ phantom for needle guidance training by
Tissue substitutes for ultrasound imaging d M. O. CULJAT et al. 869
modeling various organs using balloons filled with de-
gassed water, castor oil and castor clay (Robbins 1985).
An adult female pelvis phantom was made using a hydro-
philic polymer, water, polyester fiberfill, latex and nylon
tubing (Boyce 1993). Rowan and Pederson created
a multi-organ phantom using latex to mimic skin, agar
and graphite to mimic organs and leaking silicon tubes
to simulate internal bleeding as a training tool for the diag-
nosis of internal trauma (Rowan and Pedersen 2006).
HARD TISSUE-MIMICKING MATERIALS ANDPHANTOMS
Hard tissues are mineralized tissues with a firm inter-
cellular substance and include cortical bone, trabecular
bone, dental enamel and dentin. Bone substitutes and
phantoms have been developed primarily to evaluate
and calibrate ultrasound systems designed specifically
for detecting bone pathologies (Young et al. 1993;
Clarke et al. 1994). Ultrasound imaging of teeth has not
yet become clinically accepted, but has been the subject
of various studies because of its ability to penetrate hard
tissues and its potential as a complement to radiography
(Ghorayeb et al. 2008). Dental phantoms have been
used to guide the development of dental ultrasound
imaging systems (Blodgett 2003; Culjat et al. 2005;
Singh et al. 2007). However, because of the higher
variation in acoustic properties among hard tissues, it is
more challenging to precisely match the acoustic
properties using bone phantoms and dental phantoms
than with soft tissues. On the other hand, many hard
tissue substitutes have greater structural rigidity and
longevity than soft tissue phantoms, and therefore are
more practical for long-term use. The acoustic properties
of hard tissue substitutes are provided in Table 3.
Cortical boneCortical bone, or compact bone, has a relatively
homogeneous, compact and well-defined structure.
Cortical bone substitutes have been made using epoxy,
polymers and polymer composites, with acoustic
Table 3. Acoustic properties o
Material Tissue Velocity (m/s)At
(
Acrylic Cortical Bone 2500Carbon Fiber Plastics Cortical Bone 4400Ebonite Cortical Bone 2200Epoxy Cortical Bone 2740–3168 3.7–3Perspex Cortical Bone 2657 5.3 @Epoxy Trabecular Bone 1844–3118 7–17Polyvinyl Chloride Whole Bone 2300Dental Composite Dentin 3306 108 @Aluminum Enamel 6300Soda Lime Glass Enamel 5789 6 @ 1
properties falling within the wide range of reported values
for cortical bone (Table 1). Liquid epoxy resins and hard-
eners have been mixed to create cortical bone materials,
with one group reporting a speed of sound of 3168 m/s
and attenuation of 3.7 dB/cm at 1 MHz, and another re-
porting 2740 m/s and 3.8 dB/cm at 1 MHz (Clarke et al.
1994; Tatarinov 1998). Pores were modeled for
ultrasound porosity studies by introducing 0.8–1.5–mm–
wide cubic particles of rubber in epoxy (Clarke et al.
1994; Hodgskinson et al. 1996; Tatarinov et al. 2005)
(Fig. 3). The mineral content in bone was modeled by
burning and grinding natural bone and subsequently mix-
ing the mineral residue powder into epoxy (Tatarinov
1998).
One group exploring the use of polymers and poly-
mer composites for use as cortical bone substitutes studied
various materials within the desired speed of sound range,
including ebonite (2200 m/s), acrylic (2500 m/s), carbon
fiber plastics (4400 m/s) and fiberglass (no value reported)
(Fig. 3) (Clarke et al. 1994; Hodgskinson et al. 1996;
Tatarinov et al. 2005). Perspex, a type of acrylic glass,
was reported to have a speed of sound of 2657 m/s,
attenuation of 5.3 dB/cm MHz and density of 1180 kg/m3
(Clarke et al. 1994; Hodgskinson et al. 1996; Tatarinov
et al. 2005). Epoxies and rigid polymers and polymer
composites can sufficiently approximate the acoustic
properties of bone. However, rigid polymers and
polymer composites are simpler models, whereas epoxy-
based materials can be more closely tailored to the desired
properties and configurations.
Trabecular boneTrabecular bone, residing within cortical bone, has
a porous structure that supports vascular tissues and
contains marrow. Trabecular bone is difficult to model
because of its tortuous framework and heterogeneity. In
most cases, trabecular bone phantoms have been designed
to contain bone marrow, and therefore the acoustic prop-
erties were tailored to more closely mimic marrow than
.8 @ 1 MHz 8.4 Clarke et al. 1994; Tatarinov 19981 MHz 3.1 Clarke et al. 1994
@ 0.5 MHz – Clarke et al. 1994– – Barkmann et al. 2000
19 MHz 6.9 Singh et al. 2008– 17.0 Blodgett 2003
9 MHz 13.0 Singh et al. 2008
Fig. 3. Tubular specimens of ebonite, acrylic plastic, fiberglass and carbon fiber plastic (left) and layered cortical bonesubstitutes with rubber particles mixed in epoxy (right) (Tatarinov et al. 2005).
870 Ultrasound in Medicine and Biology Volume 36, Number 6, 2010
One group developed a trabecular bone substitute by
adding 1 mm cubic gelatin granules to liquid epoxy, de-
gassing and subsequently hardening the mixture (Clarke
et al. 1994). A range of porosities was achieved by varying
the volume of epoxy and gelatin, resulting in a speed of
sound range between 1844 and 3118 m/s and attenuation
between 7 and 17 dB/cm at 0.5 MHz (Clarke et al. 1994).
A gelatin and water mixture was used as the marrow
mimic. In another study, sunflower oil was embedded
into the pores of the material to act as a marrow substitute
(Strelitzki and Truscott 1998).
Trabecular bone phantoms have also been manufac-
tured by introducing holes into Perspex acrylic resins and
polyacetal materials, with the holes in the polyacetal filled
with water to mimic marrow (Hodgskinson et al. 1996;
Lee and Choi 2007). A phantom consisting of parallel
nylon wires, simulating trabeculae, was built in 2-D
rectangular grid arrays, with the thickness of nylon
wires chosen to match the trabecular thickness (Wear
2005). Nylon wires were previously shown to exhibit
frequency-dependent scattering similar to that exhibited
by trabecular bone (Wear 2004).
Whole boneWhole-bone phantoms include both cortical and
trabecular bone substitutes. A phantom composed of glass
beads dispersed in vulcanized silicone was used to assess
a tool for measuring mineral density in women (Young
et al. 1993). Polyvinyl chloride (PVC) tubes of varying
diameters and a speed of sound of 2300 m/s were used
as whole-bone phantoms in a study that used ultrasound
to gauge fracture risk (Barkmann et al. 2000). Axisym-
metric and nonaxisymmetric whole-bone phantoms were
made to assess cortical bone thickness using ultrasound-
guided waves, with axisymmetric phantoms built from
acrylic tubes filled with water (Moilanen et al. 2007)
and nonaxisymmetric phantoms made of PVC and filled
with butter (Moilanen et al. 2004, 2007). A fetal skull
bone phantom was built to validate the use of pulsed
Doppler ultrasound in studying cerebral vasculature and
was made from a high-density polyethylene (Vella et al.
2003). The phantom was reported to closely mimic the
fetal skull bone both acoustically and thermally (Pay
et al. 1998).
Finally, trabecular material was created using the
epoxy and sunflower oil technique, and a whole-bone
phantom was created by encasing it in a hollow Perspex
cylinder and degassing it in a vacuum chamber for studies
of osteoporotic fracture risk (Strelitzki and Truscott 1998).
Dental hard tissuesTeeth are primarily composed of enamel, the dense
fibrous ceramic composite on the outer tooth surface and
dentin, the inner structural material of a tooth that is
formed from a mineralized collagenous matrix. Enamel
was simulated using aluminum and dentin was simulated
using copper in a study that used laser-based ultrasound to
examine dental structure (Blodgett 2003). Aluminum was
found to closely match enamel in compressional (6300 m/s)
and shear (3100 m/s) wave speed of sound, as well as
acoustic impedance (17.0 MRayl), but copper was a poor
substitute for dentin.
Another group explored various glasses, ceramics
and metals as tissue substitutes for enamel. Soda lime
glass was ultimately selected because of its low attenua-
tion (6 dB/cm at 19 MHz) and comparable compressional
speed of sound (5789 m/s) and acoustic impedance (13
MRayl) (Singh et al. 2008). Self-curing resin-based dental
composite was selected as a dentin substitute in the study
over dental cements, epoxies and plastics because of its
moldability and its comparable acoustic properties (c 5
3306 m/s, A 5 108 dB/cm at 19 MHz, Z 5 6.9 MRayl)
to dentin. The group was able to prepare tooth phantoms
by injecting the composite material into a mold, curing
Tissue substitutes for ultrasound imaging d M. O. CULJAT et al. 871
it and attaching the resulting composite ‘‘dentin’’ block to
a diced glass ‘‘enamel’’ slab with composite cement.
Cracks were embedded into the composite block during
curing, and dental restorations, including silver-mercury
amalgam fillings and gold and porcelain crowns, were
also integrated into the phantoms (Culjat et al. 2005;
Singh et al. 2007). However, unlike teeth with complex
internal microstructures, the phantoms were prepared
from two monolithic sections.
DISCUSSION AND CONCLUSION
Many soft tissue-mimicking materials have been
described that have a compressional speed of sound,
density, attenuation and acoustic impedance within the
measured range of soft tissues (Tables 1 and 2). The
backscattering coefficient, nonlinearity parameter and
shear wave speed of sound (in the case of hard tissue
substitutes) have rarely been reported and therefore are
not included in the tables. Agarose-based materials have
been the most widely used and are very well characterized
in the literature. They have the advantage that they are
simple to prepare, can be tailored to vary their acoustic
properties and are able to support a uniform distribution
of scatterers. However, agarose-based tissue substitutes
are limited in size (typically ,5 cm in thickness) because
they must have high surface-to-volume ratios to properly
congeal. The longevity of agarose-based materials is
highly dependent on handling and storage.
Polyvinyl alcohol–based materials have a more
complex fabrication process, which requires multiple
freeze-thaw cycles. Like agarose-based materials, PVA
materials can be acoustically tailored and can also support
a uniform distribution of scatterers. However, PVA mate-
rials have good longevity and structural rigidity, they can
be shaped and they are therefore the most attractive choice
among the soft tissue substitutes when longevity and
stability are of interest. Of the remaining tissue substitutes
described here, each is limited either by its acoustic prop-
erties, by its stability or by its structure. Open cell foam–
based materials cannot readily be acoustically tailored, but
are unique in that localized pathologies can easily be
embedded within a phantom. Oil gel–based tissue substi-
tutes may have promise but have not been sufficiently
characterized. Most gelatin-based substitutes have been
limited by low Young’s modulus and longevity.
Soft tissue phantoms have been described that have
incorporated many of the soft tissue-mimicking materials
described before. The most common tissue-mimicking
materials used in the fabrication of solid organ phantoms
have been those based from agarose, gelatin and PVA,
with a mixture of water and glycerin as the most common
blood substitute. Processes using agar and PVA were
developed that enabled multiple layers of soft tissues to
be combined to mimic multiple structures (Madsen et al.
1982; Frayne et al. 1993; Reinertsen and Collins 2006).
However, the bulk of soft tissue phantoms have had
research efforts have focused mostly on vascular and
breast tissues.
Hard tissue phantoms have been developed using
epoxies, plastics and ceramics, and have recently begun
to advance with the advent of new materials and fabrica-
tion techniques. However, limited research has been
applied to the study of hard tissue substitutes to date,
and therefore a sufficient range of acoustic properties
has not yet been achieved. The majority of hard tissue
substitutes are simple and have good longevity, but their
acoustic properties cannot easily be tailored. Like soft
tissue substitutes, most hard tissue substitutes are homo-
geneous, and therefore lack the fibrous microstructure
and corresponding asymmetry present in hard tissues.
Of the hard tissue-mimicking materials described to
date, epoxies have the most promise. Epoxies can be
molded into the desired shape, and multiple studies have
demonstrated that epoxies can be combined with other
materials to achieve a range of acoustic properties
(Table 3) (Clarke et al. 1994; Tatarinov 1998).
Although numerous tissue phantoms are now avail-
able commercially, customized tissue substitutes continue
to have a role, primarily in the medical ultrasound research
community. Additional soft and hard tissue substitutes
will continue to be developed by academic and industry
research groups primarily because of the low cost and
design flexibility afforded by customized tissue-
mimicking materials.
Acknowledgment—Partial funding for this work provided by the Teleme-dicine and Advanced Technology Research Center (TATRC)/Depart-ment of Defense under award numbers W81XWH-07-1-0672 andW81XWH-07-1-0668.
REFERENCES
Anthony L, Aaron F. Theoretical and experimental quantification ofcarotid plaque volume measurements made by three-dimensionalultrasound using test phantoms. Med Phys 2002;29:2319–2327.
Bamber JC, Bush NL. Freehand elasticity imaging using speckle decor-relation rate. Acoust Imag 1996;22:285–292.
Barkmann R, Lusse S, Stampa B, Sakata S, Heller M, Gluer CC. Assess-ment of the geometry of human finger phalanges using quantitativeultrasound in vivo. Osteoporos Int 2000;11:745–755.
Bharadvaj BK, Mabon RF, Giddens DP. Steady flow in a model of thehuman carotid bifurcation. Part I—flow visualization. J BiomechEng 1982;15:349–362.
Blodgett DW. Applications of laser-based ultrasonics to the characteriza-tion of the internal structure of teeth. J Acoust Soc Am 2003;114:542–549.
Boote EJ, Zagzebski JA. Performance tests of Doppler ultrasound equip-ment with a tissue and blood-mimicking phantom. J Ultrasound Med1988;7:137–147.
Boyce KE. Development of a prototype anthropomorphic ultrasoundphantom: 1992 CIVCO/SDMS Innovation in Ultrasound Award.J Diagn Med Sonog 1993;9:32–37.
872 Ultrasound in Medicine and Biology Volume 36, Number 6, 2010
Brewin MP, Pike LC, Rowland DE, Birch MJ. The acoustic properties,centered on 20 MHz, of an IEC agar-based tissue-mimicking materialand its temperature, frequency and age dependence. Ultrasound MedBiol 2008;34:1292–1306.
Browne JE, Ramnarine KV, Watson AJ, Hoskins PR. Assessment of theacoustic properties of common tissue-mimicking test phantoms.Ultrasound Med Biol 2003;29:1053–1060.
Burlew MM, Madsen EL, Zagzebski JA, Banjavic RA, Sum SW. A newultrasound tissue-equivalent material. Radiology 1980;134:517–520.
Bush NL, Hill CR. Gelatine-alginate complex gel: A new acousticallytissue-equivalent material. Ultrasound Med Biol 1983;9:479–484.
Clarke AJ, Evans JA, Truscott JG, Milner R, Smith MA. A phantom forquantitative ultrasound of trabecular bone. Phys Med Biol 1994;39:1677–1687.
Culjat MO, Singh RS, Brown ER, Neurgaonkar RR, Yoon DC,White SN. Ultrasound crack detection in a simulated human tooth.Dentomaxillofac Radiol 2005;34:80–85.
D’Souza WD, Madsen EL, Unal O, Vigen KK, Frank GR,Thomadsen BR. Tissue mimicking materials for a multi-imagingmodality prostate phantom. Med Phys 2001;28:688–700.
Dabrowski W, Dunmore-Buyze J, Cardinal HN, Fenster A. A real vesselphantom for flow imaging: 3-D Doppler ultrasound of steady flow.Ultrasound Med Biol 2001;27:135–141.
Dabrowski W, Dunmore-Buyze J, Rankin RN, Holdsworth DW,Fenster A. A real vessel phantom for imaging experimentation.Med Phys 1997;24:687–693.
Davies RP, Kew J. Tissue phantom for learning US-guided vascularpunctures. J Vasc Interv Radiol 2001;12:267–268.
Dong F, Madsen EL, MacDonald MC, Zagzebski JA. Nonlinearityparameter for tissue-mimicking materials. Ultrasound Med Biol1999;25:831–838.
Edmonds PD, Ross WC, Lee ER, Fessenden P. Spatial distributions ofheating by ultrasound transducers in clinical use, indicated in a tissueequivalent phantom IEEE 1985 Ultrasonics Symposium, 1985;908–912.
Eriksson R, Persson HW, Dymling SO, Lindstrom K. Evaluation ofDoppler ultrasound for blood perfusion measurements. UltrasoundMed Biol 1991;17:445–452.
Ferrara KW, Zager BG, Sokil-Melgar JB, Silverman RH, Aslanidis IM.Estimation of blood velocity with high frequency ultrasound. IEEETrans Ultrason Ferroelectr Freq Control 1996;43:149–157.
Frayne R, Gowman LM, Rickey DW, Holdsworth DW, Picot PA,Drangova M, Chu KC, Caldwell CB, Fenster A, Rutt BK. A geomet-rically accurate vascular phantom for comparative studies of x-ray,ultrasound, and magnetic resonance vascular imaging: Constructionand geometrical verification. Med Phys 1993;20:415–425.
Fromageau J, Brusseau E, Vray D, Gimenez G, Delachartre P. Character-ization of PVA cryogel for intravascular ultrasound elasticityimaging. IEEE Trans Ultrason Ferroelectr Freq Control 2003;50:1318–1324.
Garra BS, Insana MF, Shawker TH, Russell MA. Quantitative estimationof liver attenuation and echogenicity—normal state versus diffuseliver—disease. Radiology 1987;162:61–67.
Ghorayeb SR, Bertoncini CA, Hinders MK. Ultrasonography indentistry. IEEE Trans Ultrason Ferroelectr Freq Control 2008;55:1256–1266.
Giacomini A. Ultrasonic velocity in ethanol-water mixtures. J AcoustSoc Am 1947;19:701–702.
Hall TJ, Bilgen M, Insana MF, Krouskop TA. Phantom materials forelastography. IEEE Trans Ultrason Ferroelectr Frequ Control 1997;44:1355–1365.
Hodgskinson R, Njeh CF, Whitehead MA, Langton CM. The non-linearrelationship between BUA and porosity in cancellous bone. PhysMed Biol 1996;41:2411–2420.
Hopkins RE, Bradley M. In-vitro visualization of biopsy needles withultrasound: A comparative study of standard and echogenic needlesusing an ultrasound phantom. Clin Radiol 2001;56:499–502.
Hoskins PR, Loupas T, McDicken WN. A comparison of the Dopplerspectra from human blood and artificial blood used in a flowphantom. Ultrasound Med Biol 1990;16:141–147.
Hynynen K, Clement GT, McDannold N, Vykhodtseva N, King R,White PJ, Vitek S, Jolesz FA. 500-element ultrasound phased arraysystem for noninvasive focal surgery of the brain: A preliminaryrabbit study with ex vivo human skulls. Magn Reson Med 2004;52:100–107.
International Commission on Radiation Units and Measurements. Tissuesubstitutes, phantoms, and computational modelling in medical ultra-sound. Bethesda, MD: Author; 1998.
Jansson T, Persson HW, Holmer N, Sahlstrand-Johnson P, Jannert M.Ultrasound doppler for improved diagnosis of disease in the para-nasal sinuses. 2005 IEEE Ultrasonics Symposium 2005;2:839–841.
John C. The corono-apically varying ultrasonic velocity in human harddental tissues. J Acoust Soc Am 2004;116:545–556.
Jonsson P, Sahlstrand-Johnson P, Holmer N-G, Persson HW, Jannert M,Jansson T. Feasibility of Measuring Acoustic Streaming forImproved Diagnosis of Rhinosinusitis. Ultrasound Med Biol 2008;34:228–238.
Kawase Y, Suzuki Y, Ikeno F, Yoneyama R, Hoshino K, Ly HQ,Lau GT, Hayase M, Yeung AC, Hajjar RJ, Jang I- K. Comparisonof nonuniform rotational distortion between mechanical IVUS andOCT using a phantom model. Ultrasound Med Biol 2007;33:67–73.
Kerber CW, Heilman CB. Flow dynamics in the human carotid artery: I.Preliminary observations using a transparent elastic model. AJNRAm J Neuroradiol 1992;13:173–180.
Kharine A, Manohar S, Seeton R, Kolkman RG, Bolt RA,Steenbergen W, de Mul FF. Poly(vinyl alcohol) gels for use as tissuephantoms in photoacoustic mammography. Phys Med Biol 2003;48:357–370.
Kim YT, Kim HC, Inada-Kim M, Jung SS, Yun YH, Jho MJ,Sandstrom K. Evaluation of tissue mimicking quality of tofu forbiomedical ultrasound. Ultrasound Med Biol 2009;35:472–481.
Kondo T, Kitatuji M, Kanda H. New tissue mimicking materials for ultra-sound phantoms. Ultrasonics Symposium. 2005 IEEE 2005;3:1664–1667.
Landry A, Fenster A. Theoretical and experimental quantification ofcarotid plaque volume measurements made by three-dimensionalultrasound using test phantoms. Med Phys 2002;29:2319–2327.
Lee KI, Choi MJ. Phase velocity and normalized broadband ultrasonicattenuation in polyacetal cuboid bone-mimicking phantoms. J AcoustSoc Am 2007;121:EL263–EL269.
Lerski RA, Duggan TC, Christie J. A simple tissue-like ultrasoundphantom material. Br J Radiol 1982;55:156–157.
Liu J, Roberts CJ. Feasibility studies of model and system for ultrasoniccharacterization of cornea biomechanics. Invest Ophthalmol Vis Sci2004;45:U317.
Madsen EL, Berg WA, Mendelson EB, Frank GR. Anthropomorphicbreast phantoms for qualification of investigators for ACRINProtocol 6666. Radiology 2006a;239:869–874.
Madsen EL, Frank GR, Dong F. Liquid or solid ultrasonically tissue-mimicking materials with very low scatter. Ultrasound Med Biol1998;24:535–542.
Madsen EL, Frank GR, Krouskop TA, Varghese T, Kallel F, Ophir J.Tissue-mimicking oil-in-gelatin dispersions for use in heterogeneouselastography phantoms. Ultrason Imaging 2003;25:17–38.
Madsen EL, Hobson MA, Frank GR, Shi H, Jiang J, Hall TJ, Varghese T,Doyley MM, Weaver JB. Anthropomorphic breast phantoms fortesting elastography systems. Ultrasound Med Biol 2006b;32:857–874.
Madsen EL, Zagzebski JA, Banjavie RA, Jutila RE. Tissue mimickingmaterials for ultrasound phantoms. Med Phys 1978;5:391–394.
Madsen EL, Zagzebski JA, Frank GR. An anthropomorphic ultrasoundbreast phantom containing intermediate-sized scatterers. UltrasoundMed Biol 1982;8:381–392.
Madsen EL, Zagzebski JA, Ghilardi-Netto T. An anthropomorphic torsosection phantom for ultrasonic imaging. Med Phys 1980;7:43–50.
McDicken WN. A versatile test-object for the calibration of ultrasonicDoppler flow instruments. Ultrasound Med Biol 1986;12:245–249.
Meagher S, Poepping TL, Ramnarine KV, Black RA, Hoskins PR.Anatomical flow phantoms of the nonplanar carotid bifurcation,part II: experimental validation with Doppler ultrasound. UltrasoundMed Biol 2007;33:303–310.
Tissue substitutes for ultrasound imaging d M. O. CULJAT et al. 873
Mo LY, Cobbold RS. A stochastic model of the backscattered Dopplerultrasound from blood. IEEE Trans Biomed Eng 1986;33:20–27.
Moehring MA, Ritcey JA. Sizing emboli in blood using pulse Dopplerultrasound. I. Verification of the EBR model. IEEE Trans BiomedEng 1996;43:572–580.
Moilanen P, Kilappa V, Nicholson PH, Timonen J, Cheng S. Thicknesssensitivity of ultrasound velocity in long bone phantoms. UltrasoundMed Biol 2004;30:1517–1521.
Moilanen P, Nicholson PH, Kilappa V, Cheng S, Timonen J. Assessmentof the cortical bone thickness using ultrasonic guided waves: model-ling and in vitro study. Ultrasound Med Biol 2007;33:254–262.
Nadkarni SK, Austin H, Mills G, Boughner D, Fenster A. A pulsatingcoronary vessel phantom for two- and three-dimensional intravas-cular ultrasound studies. Ultrasound Med Biol 2003;29:621–628.
Nicotra JJ, Gay SB, Wallace KK, McNulty BC, Dameron RD. Evalua-tion of a breast biopsy phantom for learning freehand ultrasound-guided biopsy of the liver. Acad Radiol 1994;1:385–387.
Oates CP. Towards an ideal blood analogue for Doppler ultrasound phan-toms. Phys Med Biol 1991;36:1433–1442.
Ophir J. Ultrasound phantom material. Br J Radiol 1984;57:1161.Patterson MS, Foster FS. The improvement and quantitative assessment
of B-mode images produced by an annular array/cone hybrid. Ultra-son Imaging 1983;5:195–213.
Pay NM, Shaw A, Bond AD. Evaluation of potential bone mimickingmaterials for ultrasound thermal test objects. Evaluation of potentialbone mimicking materials for ultrasound thermal test objects 1998;21.
Petrick J, Zomack M, Schlief R. An investigation of the relationshipbetween ultrasound echo enhancement and Doppler frequency shiftusing a pulsatile arterial flow phantom. Invest Radiol 1997;32:225–235.
Ramnarine KV, Anderson T, Hoskins PR. Construction and geometricstability of physiological flow rate wall-less stenosis phantoms.Ultrasound Med Biol 2001;27:245–250.
Ramnarine KV, Hoskins PR, Routh HF, Davidson F. Doppler back-scatter properties of a blood-mimicking fluid for Doppler perfor-mance assessment. Ultrasound Med Biol 1999;25:105–110.
Reinertsen I, Collins DL. A realistic phantom for brain-shift simulations.Med Phys 2006;33:3234–3240.
Rickey DW, Picot PA, Christopher DA, Fenster A. A wall-less vesselphantom for Doppler ultrasound studies. Ultrasound Med Biol1995;21:1163–1176.
Robertson J, Leen E, Goldberg JA, Angerson WJ, Sutherland GR,McArdle CS. Flow measurements using duplex doppler ultra-sound—hemodynamic-changes in patients with colorectal livermetastases. Clin Phys Physiol Meas 1992;13:299–310.
Robinson DE, Kossoff G. Performance tests of ultrasonic echoscopes formedical diagnosis. Radiology 1972;104:123–132.
Rowan M, Pedersen P. P2C-3 an injury mimicking ultrasound phantomas a training tool for diagnosis of internal trauma. Ultrasonics Sympo-sium, 2006 IEEE 2006;1612–1617.
Samavat H, Evans J. An ideal blood mimicking fluid for doppler ultra-sound phantoms. J Med Phys 2006;31:275–278.
Schaar JA, de Korte CL, Mastik F, van Damme LC, Krams R,Serruys PW, van der Steen AF. Three-dimensional palpography ofhuman coronary arteries. Ex vivo validation and in-patient evalua-tion. Herz 2005;30:125–133.
Sehgal CM, Bahn RC, Greenleaf JF. Measurement of the acousitcnonlinearity parameter B/A in human-tissues by a thermodynamicmethod. J Acoust Soc Am 1984;76:1023–1029.
Sheppard J, Duck FA. Ultrasonic tissue-equivalent materials using inor-gaanic gel mixtures. Br J Radiol 1982;55:667–669.
Shui G, Kim JY, Qu J, Wang YS, Jacobs LJ. A new technique formeasuring the acoustic nonlinearity of materials using Rayleighwaves. NDT&E Int 2008;41:326–329.
Singh RS, Culjat MO, Cho JC, Neurgaonkar RR, Yoon DC,Grundfest WS, Brown ER, White SN. Penetration of radiopaque
dental restorative materials using a novel ultrasound imaging system.Am J Dent 2007;20:221–226.
Singh RS, Culjat MO, Grundfest WS, Brown ER, White SN. Tissuemimicking materials for dental ultrasound. J Acoust Soc Am 2008;123:EL39–EL44.
Smith SW, Miller TM, Kisslo J. Anthropomorphic cardiac ultrasoundphantom with coronary arteries. Engineering in Medicine andBiology Society, 1991 Proceedings of the Annual InternationalConference of the IEEE 1991;13:138–139.
Smith SW, Rinaldi JE. Anthropomorphic cardiac ultrasound phantom.IEEE Trans Biomed Eng 1989;36:1055–1058.
Smith RF, Frayne R, Moreau M, Rutt BK, Fenster A, Holdsworth DW.Stenosed anthropomorphic vascular phantoms for digital subtractionangiography, magnetic resonance, and Doppler ultrasound investiga-tions. Medical Imaging 1994: Physics of Medical Imaging 1994;2163:235–242.
Sonotech. The Technology of Acoustic Scanning Gels. 2007.Strelitzki R, Clarke AJ, Truscott JG, Evans JA. Ultrasonic measurement:
An evaluation of three heel bone scanners compared with a bench-topsystem. Osteoporos Int 1996;6:471–479.
Strelitzki R, Truscott JG. An evaluation of the reproducibility and respon-siveness of four ‘state-of-the-art’ ultrasonic heel bone measurementsystems using phantoms. Osteoporos Int 1998;8:104–109.
Surry KJ, Austin HJ, Fenster A, Peters TM. Poly(vinyl alcohol) cryogelphantoms for use in ultrasound and MR imaging. Phys Med Biol2004;49:5529–5546.
Tatarinov A. Modeling the influence of mineral content and porosity onultrasound parameters in bone by using synthetic phantoms. MechCompos Mater 1998;35:147–154.
Tatarinov A, Sarvazyan N, Sarvazyan A. Use of multiple acoustic wavemodes for assessment of long bones: model study. Ultrasonics 2005;43:672–680.
Teirlinck CJ, Bezemer RA, Kollmann C, Lubbers J, Hoskins PR,Ramnarine KV, Fish P, Fredeldt KE, Schaarschmidt UG. Develop-ment of an example flow test object and comparison of five of thesetest objects, constructed in various laboratories. Ultrasonics 1998;36:653–660.
Tortoli P, Morganti T, Bambi G, Palombo C, Ramnarine KV. Noninva-sive simultaneous assessment of wall shear rate and wall distension incarotid arteries. Ultrasound Med Biol 2006;32:1661–1670.
Vella GJ, Humphrey VF, Duck FA, Barnett SB. Ultrasound-inducedheating in a foetal skull bone phantom and its dependence on beamwidth and perfusion. Ultrasound Med Biol 2003;29:779–788.
Wear KA. Measurement of dependence of backscatter coefficient fromcylinders on frequency and diameter using focused transducers—withapplications in trabecular bone. J Acoust Soc Am 2004;115:66–72.
Wear KA. The dependencies of phase velocity and dispersion on trabec-ular thickness and spacing in trabecular bone-mimicking phantoms.J Acoust Soc Am 2005;118:1186–1192.
Wells PN. Review: absorption and dispersion of ultrasound in biologicaltissue. Ultrasound Med Biol 1975;1:369–376.
Wojcik G, Szabo T, Mould J, Carcione L, Clougherty F. Nonlinear pulsecalculations and data in water and a tissue mimic. UltrasonicsSymposium, Proceedings IEEE 1999;2:1521–1526.
Xu D, Abbas S, Chan VW. Ultrasound phantom for hands-on practice.Reg Anesth Pain Med 2005;30:593–594.
Xu HX, Yin XY, Lu MD, Liu GJ, Xu ZF. Estimation of liver tumorvolume using a three-dimensional ultrasound volumetric system.Ultrasound Med Biol 2003;29:839–846.
Young H, Howey S, Purdie DW. Broadband ultrasound attenuationcompared with dual-energy X-ray absorptiometry in screening forpostmenopausal low bone density. Osteoporos Int 1993;3:160–164.
Zell K, Sperl JI, Vogel MW, Niessner R, Haisch C. Acoustical propertiesof selected tissue phantom materials for ultrasound imaging. PhysMed Biol 2007;52:N475–N484.
Zhang X, Greenleaf JF. Measurement of wave velocity in arterial wallswith ultrasound transducers. Ultrasound Med Biol 2006;32:1655–1660.